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11/1/2017 Scopus preview - Scopus - Author details (Hazmi, Ariadi)

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Hazmi, Ariadi

Universitas Andalas, Department of Electrical Engineering, Padang, Indonesia

Author ID: 23667493300

Other name formats: Hazmi, Ariad Hazmi, Hariadi

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Author History

Publication range: 2007 - Present

References: 186

Source history:

Telkomnika (Telecommunication Computing Electronics and Control)

ATMOSPHERE

ARPN Journal of Engineering and Applied Sciences

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Automatic threshold of standard deviation to reject noise

in raw data of partial discharges Waldi, E.P.,Aulia,Fernandez, R.,(...), Abral, H.,Arief, S.

2017 ARPN Journal of Engineering and Applied Sciences

Open Access

View abstract | Related documents

Thermal image, partial discharge and leakage current correlation of ceramic insulator under different contamination level

Darwison,Arief, S.,

View abstract | Related documents

Preliminary study on biogas production from POME by

DBD plasma Hazmi, A.,Desmiarti, R.,Emeraldi, P.,(...),

Edwardo,Waldi, E.P.

View abstract | Related documents

Research on positive narrow bipolar events in Padang Hazmi, A.,Emeraldi, P.,

Hamid, M.I.,Takagi, N. 2017 Proceedings - 2016 3rdInternational Conference on Information Technology, Computer, and Electrical Engineering, ICITACEE 2016

View abstract | Related documents

Characterization of positive cloud to ground flashes

observed in Indonesia Hazmi, A.,Emeraldi, P.,Hamid, M.I.,Takagi, N., Wang, D.

2017 Atmosphere

Open Access

View abstract | Related documents

Observed electric field changes of positive lightning

flashes preceded by preliminary breakdown in padang Hazmi, A.,Desmiarti, R.,Emeraldi, P., Hamid, M.I.,Takagi, N.

2017 International Journal on Electrical Engineering and Informatics

Open Access

View abstract | Related documents

Some characteristics of multiple stroke negative cloud to

ground lightning flashes in Padang Hazmi, A.,Emeraldi, P.,Hamid, M.I.,Takagi, N. 2016 International Journal onElectrical Engineering and Informatics

Open Access

View abstract | Related documents

An Optimized method of partial discharge data retrieval

technique for phase resolved pattern Waldi, E.P.,Aulia,Hazmi, A.,(...),Arief, S., Ahmad, M.H.

View abstract | Related documents

(3)

11/1/2017 Scopus preview - Scopus - Author details (Hazmi, Ariadi)

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Preliminary study on treatment of palm oil mill effluent by

sand filtration-dielectric barrier discharge system Hazmi, A.,Desmiarti, R.,Waldi, E.P., Emeraldi, P.

2016 Journal of Engineering and Technological Sciences

Open Access

View abstract | Related documents

Removal of pathogenic bacteria from water by

radio-frequency thermal plasma treatment Desmiarti, R.,Hazmi, A.,Trianda, Y.,Sari, E. 2015 Research Journal ofPharmaceutical, Biological and Chemical Sciences

View abstract | Related documents

Removal of microorganisms in drinking water using a

pulsed high voltage Hazmi, A.,Desmiarti, R.,Waldi, E.P.,Darwison 2013 Journal of Engineeringand Technological Sciences

Open Access

View abstract | Related documents Characteristics of electric field change preceding negative first return stroke produced by preliminary breakdown

View abstract | Related documents

The leakage current analysis on 20 kV suspension porcelain insulator contaminated by salt moisture and cement dust in Padang area

Aulia,David, F.,

Waldy, E.P.,Hazmi, H. 2007 Proceedings of the IEEEInternational Conference on Properties and Applications of Dielectric Materials

View abstract | Related documents

Development of a space-charge-sensing system Hazmi, A.,Takagi, N.,

Wang, D.,Watanabe, T. 2007 SensorsOpen Access

View abstract | Related documents

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Technical Program Committee:

Mochammad Facta Diponegoro University, )ndonesia

Masayuki Kurosaki Kyushu University, Japan

Trio Adiono Bandung )nstitute of Technology, )ndonesia

P. )nsap Santosa Gadjah Mada University, )ndonesia

Mauridhi (eri Purnomo Sepuluh Nopember )nstitute of Technology, )ndonesia

Khoirul Anwar Japan Advanced )nstitute of Science and Technology, Japan

Wahyudi Diponegoro University, )ndonesia

Wahyul Amien Syafei Diponegoro University, )ndonesia

Munawar Agus Riyadi Diponegoro University, )ndonesia

Sidiq Syamsul (idayat Semarang State Polytechnics, )ndonesia

Supari Semarang University, )ndonesia

Slamet Riyadi Soegijapranoto Katholic University, )ndonesia

M. (adin Sultan Agung )slamic University, )ndonesia

Onil Nazra Persada CEA, France

Zolkafle Buntat Universiti Teknologi Malaysia

Taufik California Polytechnic State University, USA

(ashim Uledi )ddi University of Dar es Salaam, Tanzania

Aris Triwiyatno Diponegoro University, )ndonesia

Pandu Sandi Pratama Pusan National University, South Korea

Razali )smail Universiti Teknologi Malaysia, Malaysia

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T

ABLE OF

C

ONTENTS

Keynote Speakers

1 Hydro, Solar, and Wind Energy as Potential Electrical Power Plant in Indonesia - Past Conditions and Future Prospects

Yanuarsyah Haroen

2 Low Latency Network-on-Chip Router Using Static Straight Allocator

Alireza Monemi, Chia Yee Ooi, Maurizio Palesi, Muhammad Nadzir Marsono

10 Smart Video-Based Surveillance: Opportunities and Challenges from Image Processing Perspectives

Syed Abdurrahman

Electronic Circuit and Control

11 Human Tracking Application in a Certain Closed Area Using RFID Sensors and IP Camera

Daniel Patricko Hutabarat, Darma Patria, Santoso Budijono, Robby Saleh

17 Designing and Implementation of Autonomous Quadrotor as Unmanned Aerial Vehicle

Felix Yustian Setiono, Anthony Candrasaputra, Tobias Bimo Prasetyo, Kho Lukas Budi Santoso

21 Multi Channel Electromyography (EMG) Signal Acquisition using Microcontroller with Rectifier

Florentinus Budi Setiawan, S. Siswanto

25 ECG Signal Processing using Offline-Wavelet Transform Method based on ECG-IoT Device

M. Faizal Amri, Muhammad Ilham R, Arjon Turnip

31 Trans-impedance Amplifier (TIA) Design for Visible Light Communication (VLC) using Commercially Available OP-AMP

Syifaul Fuada, Angga Pratama Putra, Yulian Aska, Trio Adiono

37 Robot ARM Controlled by Muscle Tension Based on Electromyography and PIC18F4550

Ricky Fajar Adiputra, Florentinus Budi Setiawan

42 A Low Cost Anthropomorphic Prosthetic hand Using DC Micro Metal Gear motor

Mochammad Ariyanto, M. Munadi, Gunawan D. Haryadi, Rifky Ismail, Jonny A. Pakpahan, Khusnul A. Mustaqim

47 New Watershed Segmentation Algorithm based on Hybrid Gradient and Self-Adaptive Marker Extraction

Yuan Li, Yu Qingsong, Shen Chaomin, Hu Wenxin

52 Variations on Load and Distance Controller for Modern Elevator with Fuzzy

Ainil Syafitri, Iwa Garniwa MK, Ridwan Gunawan, I Made Ardita

56 Fuzzy-PID Simulations on Ropeless Elevator Performance

Ainil Syafitri, Iwa Garniwa MK, Ridwan Gunawan, I Made Ardita

60 A Simple Proportional plus PD Sign for Asymptotically Stable Robot Manipulators

Adha Imam Cahyadi, Samiadji Herdjunanto, H. Herianto

64 Arrival Time Field Based Path Planning Algorithm for Mobile Robot

Imaduddin A. Majid, Adha Imam Cahyadi, Igi Ardiyanto, Muhammad Saifussalam

68 Design of Soft Contact Lens Indexer Inspection Semi-Automatic

Didi Istardi, Kemas Syaiful

74 Yuarm: A Low Cost Android Platform for Vision Based Manipulators Control

Sisdarmanto Adinandra, Dany Erfawan

79 Development of Unmanned Aerial Vehicle (UAV) Ornithopter with Wireless Radio Control

Farika T. Putri, Mochammad Ariyanto, Ismoyo Haryanto, Moh. Arozi, Wahyu Caesarendra, M. Rizki Ibrahim Hanan

85 Comparison Methods of Edge Detection for USG Images

(16)

89 Ultrasonic Signal Denoising Based on Wavelet Haar Decomposition Level

H. Herlinawati, Umi Murdika, Grienda Elan, Titin Yulianti

95 Sliding Mode Control for Therapeutic Pool Model Control System

M. Munadi, Henry Kristianto, Mochammad Ariyanto, Ismoyo Haryanto, Hari Peni Julianti

100 Experiment of Networked Control System (NCS) Using Network Emulator

Indra Sakti, Dicky Rianto Prajitno

106 Brainwave-Controlled Applications with the Emotiv EPOC Using Support Vector Machine

Ha Hoang Kha, Vo Anh Kha, Dinh Quoc Hung

112 Development of Hovercraft Prototype with Stability Control System using PID Controller

Munawar A. Riyadi, Lazyo Rahmando, Aris Triwiyatno

117 Design of Color Based Object Sorting Through Arm Manipulator with Inverse Kinematics Method

S. Sumardi, Lanang Febriramadhan, Aris Triwiyatno

123 Designing Internal-External Control Method for Delta Robot Prototype to Manipulate Non-Linear Move-ment Object

Aris Triwiyatno, Muhammad Fikko Fadjrimiratno, S. Sumardi

129 Real Time Classification of SSVEP Brain Activity with Adaptive Feedforward Neural Networks

Arjon Turnip, M. Ilham Rizgyawan, Dwi Esti K., Jasman Pardede, Sandi Yanyoan, Edi Mulyana

134 Fuzzy-Mamdani Inference System in Predicting the Correlation Between Learning Method, Discipline and Motivation with Student’s Achievement

J. Juningtyastuti, Fransiskus Allan Gunawan

Electric and Power System

140 Investigation of Temperature Rise Considering the Stator Parameters in a High-Speed Spindle Motor

Wawan Purwanto, Jerry Chih Tsong Su

147 Voltage Balancing Circuits for Five-Level Power Inverter With A Single DC Voltage Source

S. Suroso, Abdullah Nur Aziz

151 The Use of Neural Network (NN) to Predict Voltage Drop during Starting of Medium Voltage Induction Motor

Fidelis Galla Limbong

156 Research on Positive Narrow Bipolar Events in Padang

Ariadi Hazmi, Primas Emeraldi, M. Imran Hamid, Nobuyaki Takagi

160 Minimization of Cogging Torque Based on Different Shape of Anti-Notch Method

H. Herlina, Rudy Setiabudy, Uno Bintang Sudibyo

164 Investigation of the Influence of Variations in the Number and Width of Anti-Notch depending on Cogging Torque Reduction

Rudy Setiabudy, H. Herlina

168 Voltage Drop Simulation at Southern Sulawesi Power System Considering Composite Load Model

Ardiaty Arief, Muhammad Bachtiar Nappu

172 Analytical Design of Sea Wave Energy Power Plant Using Tubular Linear PM Generator in Southern Coast of Yogyakarta, Indonesia

Budi Azhari, Fransisco Danang Wijaya, Dewangga Adhyaksa, Wassy Prawinnetou

177 Reduction on Cogging Torque in Dual Stator Radial Flux Permanent Magnet Generator for Low Speed Wind Turbine

Adeguna Ridlo Pramurti, Eka Firmansyah, S. Suharyanto

181 Network Losses Reduction Due To New Hydro Power Plant Integration

Muhammad Bachtiar Nappu, Muhammad Imran Bachtiar, Ardiaty Arief

186 Electrical and Temperature Correlation to Monitor Fault Condition of ZnO Surge Arrester

N. Novizon, Zulkurnain Abdul-Malek

191 Discrimination of Particle-Initiated Defects in Gas-Insulated System Using C4.5 Algorithm

Firmansyah Nur Budiman, Elvira Sukma Wahyuni

197 Enhanced Fault Ride – Through Ability of DFIG-Based Wind Energy System Using Superconducting Fault Current Limiter

(17)

202 Design of Photovoltaic BLDC Motor-Water Pump System with Single Converter

Slamet Riyadi

208 Integrated LC Resonant Converter and Silent Discharge Ozonizer for Colour Removal

Mochammad Facta, H. Hermawan, Zolkafle Buntat

213 A Prototype of Multistage Dynamic Braking of Three Phase Squirrel Cage Induction Motor

Tejo Sukmadi, Syauqie Candra Buana, Trias Andromeda, Mochammad Facta

216 Application of Dielectric Barrier Discharge Plasma for Reducing Chemical Oxygen Demand (COD) on Industrial Rubber Waste Treatment

Abdul Syakur, Badrus Zaman, F. Fauzan, Nur Jannah, Nurmaliakasih Dias Yunita

Information and Computer Technologies

220 Calculation of Phantom Volume for Computed Tomography (CT) Scan Images

Kusworo Adi, Catur Edi Widodo, Aris Sugiharto, Qidir Maulana B.S., Adi Pamungkas

224 Design and Development of Android-based Cloud ECG Monitoring System

Muhammad Ilham Rizqyawan, M. Faizal Amri, Rian Putra Pratama, Arjon Turnip

229 Designing Framework for Software Reuse Maturity Improvement

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RESEARCH ON POSITIVE NARROW

BIPOLAR EVENTS IN PADANG

Ariadi Hazmi, Primas Emeraldi, M. Imran Hamid

Dept. of Electrical Engineering Andalas University

Padang, Indonesia ariadi@ft.unand.ac.id

Nobuyuki Takagi

Dept. of Electrical and Electronic Engineering Gifu University

Gifu City, Japan

1-1 Yanagido, Gifu 501-1193, Japan

Abstract In this study, we have examined electric field

records from 10 thunderstorm days containing 13 positive narrow bipolar pulses (PNBPs). It was found that PNBP occurrences have a strong relationship with thunderstorm activities. The mechanism of the NBPs was very different from intracloud (IC) and cloud-to-ground (CG) flashes. We also found that the AM values of rise time, full width at maximum time, zero crossing time, overshoot time, pulse duration and overshoot to peak amplitude ratio of the PNBPs were 1.64 μs, 1.32 μs, 9.38 μs, 15.06 μs and 0.31 μs, respectively. The pulse duration range was from 8.45 to 29.06 μs. Comparison with values from previous studies reported by other researchers showed that the mentioned parameters had no strong relationship with latitude or geographic location.

Keywords—narrow bipolar pulse; cloud flash; ground flash; thunderstorm; lightning

I. INTRODUCTION

Narrow bipolar pulses (NBPs) are identified as one of the intracloud (IC) lightning discharge activities inside thunderclouds. However, the physical mechanism of NBPs remains a mystery. Many researchers have reported that there were two types of NBPs, namely positive narrow bipolar pulses (PNBP) and negative narrow bipolar pulses (NNBP). NBPs have strong radio frequency radiation at several MHz and a short duration with zero crossing (initial positive half cycle) and overshoot (negative half cycle) within several microseconds, followed by or not followed by any other signals [1-4]. NBPs may not be related to ground and cloud flash activities and originate inside the most active thundercloud areas [2]. PNBPs usually occur at lower latitudes than NNBPs. In addition, PNBP occurrences are rare compared to NNBP events [5]. This study is to clarify the relationship between thunderstorm activity and PNBP occurrence. We examined an electric field change data set with 13 PNBPs that were recorded during thunderstorm days in 2015. The characteristics of the PNBPs were statistically analyzed based on electric field change as presented in this paper. All data were also compared to previous researches at different locations and latitudes.

II. OBSERVATION AND DATA

The electric field records containing the PNBPs presented here were recorded from January to December 2015 in Padang, Indonesia (0° N) on 10 thunderstorm days using an electric field mill and a broadband electric field fast antenna. Both electric field sensors on the rooftop of the Electrical Engineering Department Building of Andalas University were located at 13 km from Padang Beach, Indian Ocean at an altitude of 317 m above sea level. The fast antenna with parallel flat-plate configuration was used to detect electric field changes in the thunderclouds. The fast antenna was connected to an amplifier and integrator with a time constant of 100 ms. Furthermore, all signals sensed by this antenna were recorded by a digitizer with a sample rate in the range of 1-4 MS/s and a record length of 250 ns - 1 s. To ensure that the strong electric field of lightning was recorded, the digitizer was set to window trigger mode at a trigger level of 1 V and a pretrigger time of 30% of the record length. The electric field measurement system used was similar to the one used in Hazmi et al. [6-7].

III. RESULTS AND DISCUSSION

In this study, 13 PNBP occurrences were analyzed. A summary of the PNBP events can be seen in Table 1. There are two types of PNBP events; for convenience, type A is called isolated PNBP to indicate that there are no other IC lightning occurrences, while type B is called non isolated PNBP which indicates that the occurrences are preceded or followed by other IC lightning occurrences, as displayed in Figures 1 and 2. The occurrence percentage of type A (46%) was slightly smaller than that of type B (54%). From Table 1, the PNBPs occurred during day and night time with the duration of the thunderstorms varying from 126 to 844 minutes. The background electric field changes of the thunderstorms recorded by an electric field mill sensor for negative and positive polarities varied between 0.284-4.096 kV/m and 0.364-4.094 kV/m, respectively. This indicates that the PNBPs occurred inside the most active thundercloud areas with high electric field. Our observation results were a good agreement with observation of Smith et al. [2]. However, PNBPs also occurred when the thunderstorms detected had a lower electric field, for example thunderstorm numbers 8 and 11 in Table 2. This may be due to the different distance between the PNBPs

Proc. of 2016 3rdInt. Conf. on Information Tech., Computer, and Electrical Engineering (ICITACEE), Oct 19-21st, 2016, Semarang, Indonesia

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and the electric field mill sensor. The more distant the measurement, the smaller the electric field magnitude recorded by the electric field mill sensor. We did not find that any of the PNBP events were accompanied by CG flash events. Thus, there is not strong relationship between PNBP, IC and CG flash occurrence.

The physic sign convention was used to examine the electric field changes in this study. An expanded PNBP is shown in Figure 3. In addition, the studied parameters in this research were full width at maximum time (0-100%), rise time (10-90%), zero crossing time, overshoot time, pulse duration and overshoot to peak amplitude ratio, as shown in Figure 3. The characteristics of the PNBPs are summarized in Table 2.

Fig. 1. A typical isolated PNBP E-field waveform.

.

The full width at maximum time (Tr1) is the time interval

that relates to the values of 0% and 100% of the peak

amplitude of the signal. This parameter is important to measure the initial transient signal of a PNBP. The minimum, maximum, arithmetic mean (AM) and geometric mean (GM) values of the full width at maximum time were 3.24 ± 1.20 μs, 3 μs, respectively.

The rise time (Tr2) is the time interval that relates to the

values of 10% and 90% of the peak amplitude signal. The AM

and GM values of PNBP rise time were 1.64 ± 0.51 μs and

1.56 μs, respectively, with minimum and maximum values of

0.89 μs and 2.65 μs, respectively. Comparing these values to those from other researchers, our AM value was smaller than that of Karunarathne et al. [8], Ahmad et al. [9] and Sharma et al. [10]. Their results were 2.6 μs, 2.7 μs and 2.6 μs, respectively. However, our AM value was larger than that of Medelius et al. [11] and Gunasekara et al. [12] with obtained results of 1.54 μs and 1.38 μs, respectively. The difference may be due to data limitations in this study.

Fig. 2. A typical non isolated PNBP E-field waveform. TABLE 1.SUMMARY OF 10 THUNDERSTORM DAYS RECORDED IN PADANG FROM JANUARY TO DECEMBER 2015.

No File Name dd/mm/yy Date Local Time (hh:mm:ss) Type

Thunderstorm in 24 hours

Duration (min) Maximum E-field polarity (kV/m)

Negative Positive

1 20140526-0001 (25369) 30/01/2015 6:21:51 A

126 -4.096 4.094 2 20140526-0001 (25370) 30/01/2015 6:22:45 B

3 20140526-0001 (25539) 05/02/2015 19:10:27 A

636 -3.668 3.368 4 20140526-0001 (25554) 05/02/2015 19:33:55 B

5 20140526-0001 (25573) 16/02/2015 12:55:38 B 150 -4.096 2.926 6 20140526-0001 (26674) 08/03/2015 2:27:38 B 192 -1.668 2.756 7 20140526-0001 (27162) 14/03/2015 22.18:17 B 436 -4.096 4.094 8 20140526-0001 (27299) 18/03/2015 19:54:53 B 844 -0.284 0.364 9 20140526-0001 (28048) 24/03/2015 22:32:12 A 678 -4.096 3.874 10 20140526-0001 (30179) 10/04/2015 15:47:19 B 802 -3.202 2.228 11 20140526-0001 (30226) 15/04/2015 1:07:08 A 561 -1.378 1.856 12 20140526-0001 (31524) 11/12/2015 19:11:39 A

642 -4.096 4.094 13 20140526-0001 (31527) 11/12/2015 19:20:42 A

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The zero crossing time (Tz) is defined as the time difference

from the first zero point to the next zero point, represented by zero crossing of the signal. The zero crossing time varied from 3.72 to 7.03 μs with AM and GM values of 5.23 ± 1.14 μs and

5.11 μs. The AM values from previous studies in other

latitudes, as reported by Gunasekara et al. [12], Karunarathne et al. [8], Nag et al. [13], Ahmad et al. [9], Sharma et al. [10] and Cooray and Lundquist [14], were 4.66 μs, 9.9 μs, 5.6 μs, 6.5 μs, 5.78 μs, and 13 μs, respectively. The zero crossing time at the same latitude had different values as reported by Gunasekara et al. [12] and Sharma et al. [10]. It was clear that the AM value did not depend on latitude.

The overshoot time (To) is the time interval between the

first zero crossing point and the end signal to reach the next zero crossing point. It varied from 3.71 to 25.23 μs. The mean value was 9.38 ± 6.55 μs with a GM value of 8.01 μs.

Fig. 3. The expanded narrow bipolar pulse E-field waveform.

The pulse duration is the total time interval that corresponds to the positive half cycle and the negative half cycle (overshoot) of the signal. It had an AM value of 15.06 ± 6.38 μs and a GM value of 13.90 μs, while it ranged from 8.45

to 29.06 μs. The AM values from other researchers, i.e.

Gunasekara et al. [12], Nag et al. [13], Ahmad et al. [9], Sharma et al. [10] and Cooray and Lundquist [14], were 16.42

μs, 23 μs, 30.2 μs, 13.3 μs, and 75 μs, respectively. It was found that the AM value did not depend on latitude. The different results may be due to the specific characteristics of the electric field sensor system and thunderstorm type.

TABLE 2. SUMMARY OF OBSERVED PNBP PARAMETERS.

determined by comparing peak overshoot to initial peak of

signal amplitude. The minimum, maximum, standard deviation, AM and GM values of this ratio were 0.17 μs, 0.41

μs, 0.07 μs, 0.31 μs and 0.30 μs. The results from previous researches, as reported by Gunasekara et al. [12], Nag et al. [13], Ahmad et al. [9], Sharma et al. [10] and Cooray and Lundquist [14], were 0.37 μs, 0.17 μs, 0.27 μs, 0.35 μs, and 0.30 μs, respectively. Our mean value showed was the same as in previous researches, except from Nag et al. [13]. We predict that the difference in this parameter was influenced by differences in season and charge distribution of the thunderstorms.

IV. CONCLUSION

10 thunderstorm days containing 13 PNBPs were examined based on electric field records. The thunderstorm activities did not always cause PNB events. However, it was found that the PNBP occurrences had a strong relationship with thunderstorm activities. The PNBP mechanism is very different from IC and CG flashes. From our observations, the AM value of rise time, full width of maximum time, zero crossing time, overshoot, pulse duration and overshoot to peak amplitude ratio of PNBPs were 1.64 μs, 1.32 μs, 9.38 μs, 15.06 μs and 0.31 μs, respectively. Comparison with previous studies, as reported by other researchers, suggests that the mentioned parameters do not depend on latitude or geographic location. The differences may be due to differences in thunderstorm types, seasonal conditions and instrumentation system characteristics. Further research is needed to gain a better understanding of the physical mechanism of narrow bipolar events (NBE).

ACKNOWLEDGMENT

This work was supported by International Research Collaboration and Scientific Publication grant, No. 04/H.16/KLN-PI/LPPM/2016, Indonesia. The authors to thank Budi Harianto for helping to analyze data.

REFERENCES

[1] Willett, J.C., Bailey, J.C., Krider, E.P., 1989. A class of unusual lightning electric ¿eld waveforms with very strong HF radiation. J. Geophys. Res. 94, 16255–16267. http://dx.doi.org/10.1029/ JD094iD13p16255.

[2] Smith, D.A., Shao, X.M., Holden, D.N., Rhodes, C.T., Brook, M., Krehbiel, P.R., Stanley, M., Rison, W., Thomas, R.J., 1999. A distinct class of isolated intracloud lightning discharges and their associated radio emissions. J. Geophys. Res. 104, 4189–4212. http://dx.doi.org/ 10.1029/1998JD200045.

[3] Smith, D.A., Heavner, M.J., Jacobson, A.R., Shao, X.M., Massey, R.S., Sheldon, R.J.,J. Clerk Maxwell, A Treatise on Electricity and Magnetism, 3rd ed., vol. 2. Oxford: Clarendon, 1892, pp.68-73. Weins, K.C., 2004. A method for determining intracloud lightning and ionospheric heights from VLF/LF electric ¿eld records. Radio Sci. 39, RS1010. http://dx.doi.org/10.1029/2002RS002790.

[4] Eack, K.B., 2004. Electrical characteristics of narrow bipolar events. Geophys. Res. Lett. 31, L20102. http://dx.doi.org/10.1029/ 2004GL021117.

[5] Ahmad, M.R., Esa, M.R.M., Cooray, V., Baharudin, Z.A., Hettiarachchi, P., 2015. Latitude dependence of narrow bipolar pulse emissions. Journal of Atmospheric and Solar-Terrestrial Physics 128, 40–45.

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[6] Hazmi, A., Hendri, Z., Mulyadi S., Tesal, D., Wang, D., Takagi, N., 2013. Characteristics of electric field change preceding negative first return stroke produced by preliminary breakdown. International Conference on Information Technology and Electrical Engineering: "Intelligent and Green Technologies for Sustainable Development", ICITEE 2013, 322-325.

[7] Hazmi, A., Emeraldi, P., Hamid., M.I., Takagi, N., 2016. Some characteristics of multiple stroke negative cloud to ground lightning flashes in Padang. International Journal on Electrical Engineering and Informatics - Volume 8, Number 2, 438-450.

[8] Ahmad, N.A., Fernando, M., Bahaudin, Z.A., Cooray, V., Ahmad, H., Malek, Z.A., 2010. Characteristics of narrow bipolar pulses observed in Malaysia. J. Atmos. Sol. Terr. Phys. 72, 534–540. http://dx.doi.org/ 10.1016/j.jastp.2010.02.006.

[9] Karunarathne, S., Marshall, T. C., Stolzenburg, M. and Karunarathna, N., 2015. Observations of positive narrow bipolar pulses, J. Geophys. Res. Atmos., 120, doi:10.1002/2015JD023150.

[10] Sharma, S.R., Fernando, M., Cooray, V., 2008. Narrow positive bipolar radiation from lightning observed in Sri Lanka. J. Atmos. Sol. Terr. Phys. 70, 1251–1260. http://dx.doi.org/10.1016/j.jastp.2008.03.002. [11] Medelius, P.J., Thomson, E.M., Pierce, J.S., 1991. E and DE/DT wave

shapes for narrow bipolar pulses in intra-cloud lightning. In: Proceedings of the International Aerospace and Ground Conference on Lightning and Static Electricity, NASA Conference Publ., vol. 3106, pp. 12-1–12-10.

[12] Gunasekara, T.A.L.N, Fernando, M., Sonnadara, U., Cooray, V., 2016. Characteristics of Narrow Bipolar Pulses observed from lightning in Sri Lanka, Journal of Atmospheric and Solar-Terrestrial Physics 138-139, 66–73.

[13] Nag, A., Rakov, V.A., Tsalikis, D., Cramer, J.A., 2010. On phenomenology of compact intracloud lightning discharges. J. Geophys. Res. 115, D14115. http://dx.doi.org/10.1029/2009JD012957.

[14] Cooray, V., Lundquist, S., 1985. Characteristics of the radiation ¿elds from lightning in Sri Lanka in the tropics. J. Geophys. Res. 90, 6099– 6109. http://dx.doi.org/10.1029/JD090iD04p06099.

Gambar

Fig. 2. A typical non isolated PNBP E-field waveform.
Fig. 3. The expanded narrow bipolar pulse E-field waveform.

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